• Aucun résultat trouvé

The influence of synoptic circulations and local processes on temperature anomalies at three French observatories.

N/A
N/A
Protected

Academic year: 2021

Partager "The influence of synoptic circulations and local processes on temperature anomalies at three French observatories."

Copied!
47
0
0

Texte intégral

(1)

HAL Id: hal-01372848

https://hal-insu.archives-ouvertes.fr/hal-01372848v2

Submitted on 26 Jun 2017

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

The influence of synoptic circulations and local processes on temperature anomalies at three French observatories.

Cheikh Dione, Fabienne Lohou, Marjolaine Chiriaco, Marie Lothon, Sophie Bastin, Jean-Luc Baray, Pascal Yiou, Aurélie Colomb

To cite this version:

Cheikh Dione, Fabienne Lohou, Marjolaine Chiriaco, Marie Lothon, Sophie Bastin, et al.. The influ- ence of synoptic circulations and local processes on temperature anomalies at three French observa- tories.. Journal of Applied Meteorology and Climatology, American Meteorological Society, 2017, 58 (1), pp.141-158. �10.1175/JAMC-D-16-0113.1�. �hal-01372848v2�

(2)

The influence of synoptic circulations and local processes on temperature

1

anomalies at three French observatories

2

Cheikh DIONE1∗†, Fabienne LOHOU1, Marjolaine CHIRIACO2, Marie LOTHON1, Sophie

3

BASTIN2, Jean-Luc BARAY3, Pascal YIOU4and Aur´elie COLOMB3

4

(1) Laboratoire d’A´erologie, Universit´e de Toulouse, CNRS, UPS, France.

5

(2) LATMOS/IPSL, UVSQ Universit´e Paris-Saclay, UPMC Univ. Paris 06, CNRS, Guyancourt, France.

6

7

(3) Laboratoire de M´et´eorologie Physique, UMR 6016 Universit´e Blaise Pascal/CNRS, Clermont Ferrand, France.

8

9

(4) Laboratoire des Sciences du Climat et de l’Environnement, UMR8212 CEA-CNRS-UVSQ, Universit´e Paris - Saclay & IPSL, Gif-Sur-Yvette, France.

10

11

Corresponding author address: Dr. Cheikh DIONE, Centre de Recherches Atmosph´eriques, 8 route de Lannemezan, 65300 Campistrous, France.

12

13

E-mail: Cheikh.dione@aero.obs-mip.fr

14

Current affiliation: Laboratoire d’A´erologie, Universit´e de Toulouse, CNRS, UPS, France.

15

LaTeX File (.tex, .sty, .cls, .bst, .bib) Click here to download LaTeX File (.tex, .sty, .cls, .bst, .bib) dione_et_al_2016.tex

(3)

ABSTRACT

The relative contribution of the synoptic-scale circulations to local and mesoscale processes was quantified in terms of the variability of middle lat- itude temperature anomalies from 2003 to 2013 using meteorological vari- ables collected from three French observatories and reanalyses. Four weather regimes were defined from sea level pressure anomalies using National Center for Environmental Prediction (NCEP) reanalyses with a K-means algorithm.

No correlation was found between daily temperature anomalies and weather regimes, and the variability of temperature anomalies within each regime was large. It was therefore not possible to evaluate the effect of large scales on temperature anomalies by this method. An alternative approach was found with the use of the analogues method: the principle being that for each day of the considered time series, a set of days which had a similar large-scale 500 hPa geopotential height field within a fixed domain were considered. The ob- served temperature anomalies were then compared to those observed during the analogue days: the closer the two types of series, the greater the mark of the large scale. This method highlights a widely predominant influence of the large-scale atmospheric circulation on the temperature anomalies. It showed a potentially larger influence of the Mediterranean Sea and orographic flow on the two southern observatories. Low-level cloud radiative effects substantially modulated the variability of the daily temperature anomalies.

16

17

18

19

20

21

22

23

24

25

26

27

28

29

30

31

32

33

34

35

(4)

1. Introduction

36

Temperature fluctuations in France and, more generally, Western European are largely connected

37

to large-scale weather regimes. However, the processes linking atmospheric variability to surface

38

temperature may vary with the season. Cattiaux et al. (2010) used 500 hPa geopotential height to

39

define weather regimes influencing Europe and found that the cold winter of 2010 was associated

40

with a large occurrence of the negative phase of the North Atlantic Oscillation (NAO) weather

41

regime. In summer, major heat waves over France and the UK are generally linked to persistent

42

anticyclonic conditions (such as those in 2003) (Cassou et al. 2005; Yiou et al. 2008). They

43

may also be linked to Atlantic low pressure, which leads to southerly flows (such as those seen

44

in 2015), with amplification by soil moisture-temperature and boundary-layer feedbacks (Sch¨ar

45

et al. 2004; Seneviratne et al. 2006; Fischer et al. 2007b; Vautard et al. 2007; Quesada et al. 2012;

46

Miralles et al. 2014). Warm winters are linked to a zonal westerly flow (such as in 2007 and 2014)

47

(Luterbacher et al. 2007), which can be amplified by land albedo and cloud radiative effects. The

48

role of such amplifying factors was investigated mainly with regional model simulations (Zampieri

49

et al. 2009; Stegehuis et al. 2013; Seneviratne et al. 2004; Stefanon et al. 2014), but it was proven

50

necessary to use high-resolution observations to validate such an approach, since models seemed

51

to exacerbate the role of these factors over Europe (Cheruy et al. 2014; Bastin et al. 2016). For

52

example, Chiriaco et al. (2014), using a combination of space and ground-based observations and

53

twin simulations, showed that the heat wave that occurred over Northern Europe in July 2006

54

was linked to specific large-scale conditions favoring a low cloud deficit over this area and was

55

amplified by dry soil, which contributed to about 40% of the anomaly.

56

As for the weather regimes, a flow analogue method was also used to study the seasonal vari-

57

ability of surface temperature anomalies over Europe (Cattiaux et al. 2010; Chiriaco et al. 2014;

58

(5)

Vautard and Yiou 2009; Yiou et al. 2007). Cattiaux et al. (2010) found a larger positive depar-

59

ture of observed temperatures from flow analogues for minimum than for maximum temperatures.

60

They observed a maximum departure over the Alps region. Spatial variability and underestimation

61

of observed temperature anomalies by reconstructed temperature anomalies suggest an important

62

role of the smaller scale processes concerning temperature anomalies. France is located in a tran-

63

sitional region between subtropical influences and Atlantic perturbations. It covers an area where

64

climatic model predictions have suggest significant uncertainty, with large scatter in temperature

65

and precipitation due to different sensitivities to local processes (Bo´e and Terray 2014). For these

66

reasons, it is useful to employ observational data to quantify the influence of large-scale atmo-

67

spheric circulations relative to those of local processes to help explain the variability of daily

68

temperature anomalies across France.

69

Our study aims to quantify the relative contributions of large-scale atmospheric circulations and

70

of local processes on the variability of temperature anomalies at three observatories located in

71

France. For this, we shall evaluate specific issues : (i) the effect of weather regimes on daily tem-

72

perature anomalies by use of the classification of weather regimes defined from sea level pressure

73

(Yiou and Nogaj 2004), and (ii) the capability of local processes to amplify or reduce temperature

74

anomalies by use of flow analogue atmospheric circulations based on geopotential height at 500

75

hPa (Yiou et al. 2007). Our analysis is based on a series of meteorological variables (temperature,

76

wind and radiation) observed at three observatories from ROSEA (R´eseau d’Observatoires pour

77

la Surveillance de l’Eau Atmosph´erique) national network. It is also based on reanalyses (NCEP

78

and ECMWF).

79

The manuscript is organized as follows. In section 2, the three ROSEA observatories, the cor-

80

responding datasets, the large-scale diagnostic and the methodological approach are presented.

81

(6)

Section 3 presents the analysis of large-scale conditions versus local processes using flow ana-

82

logues. Conclusions appear in section 4.

83

2. Data and methodology

84

a. Observatories

85

In this study, we use surface observations from three observatories (SIRTA (Site Instrumen-

86

tal de Recherche en T´el´edetection Active), COPDD (C´ezeaux-Opme-Puy De Dˆome) and P2OA

87

(Plateforme Pyr´en´eenne de l’Observation de l’Atmosph`ere)) from the five ROSEA network ob-

88

servatories, located across varied landscapes along a North-South transect across France (Figs. 1a

89

and 1b).

90

1) SIRTA

91

The northern observatory of ROSEA is known as SIRTA (48.7N-2.2E and 160 m elevation)

92

(Haeffelin 2005). SIRTA is located on a plateau in a suburban area in Palaiseau, 20 km south-

93

west of Paris (Fig. 1a). It is dedicated to the research of physical and chemical processes in the

94

atmosphere, mainly using remote sensing. Since 2002, observations of precipitation, water va-

95

por, clouds, meteorological variables, atmospheric gases, solar radiation, and wind power have

96

been collected. More details concerning the SIRTA observatory can be found in Haeffelin (2005)

97

or on the following website: http://sirta.ipsl.polytechnique.fr/sirta.old/. Quality control and ho-

98

mogenization of the data yielding a uniform hourly time-resolution was undertaken at SIRTA for

99

the entire observation period (Chiriaco et al. 2014; Cheruy et al. 2013). This project, named

100

SIRTA-ReOBS, provides a single netCDF file with more than 40 variables from 2003 to 2013

101

(http://sirta.ipsl.polytechnique.fr/sirta.old/reobs.html).

102

(7)

2) C ´EZEAUX-COPDD

103

The COPDD observatory is located in the Auvergne region, in the center of France (Fig. 1a)

104

where various in situ and remote sensing instruments continuously measure the atmospheric dy-

105

namics, radiation, atmospheric gases, cloud microphysical variables and aerosols. This observa-

106

tory is composed of three instrumented sites: C´ezeaux (at an altitude of 394 m, an urban site,

107

Opme (at an altitude of 680 m), and Puy-De-Dˆome (at an altitude of 1465 m). In this study, we

108

use the meteorological variables collected at the C´ezeaux site in order to obtain relatively similar

109

terrain across the three sites. The C´ezeaux site (45.47N-3.05E) is located on a plain on the cam-

110

pus of Blaise Pascal University in Clermont Ferrand. Since 2002, meteorological variables have

111

been measured at this site. More details concerning the COPDD observatory can be found on the

112

following website; http://wwwobs.univ-bpclermont.fr/SO/mesures/index.php.

113

3) CRA-P2OA

114

The P2OA observatory is the southern most site (Fig. 1a). It is located in the Midi-Pyren´ees

115

region and is composed of two sites from the Observatoire Midi Pyr´en´ees (OMP): the Atmo-

116

spheric Research Center (CRA) in Lannemezan (43.13N-0.369E at an altitude of 600 m), and

117

the “Pic du Midi” (43.13N-0.37E at an altitude of 2877 m). On this platform, various in situ

118

and remote sensing instruments continuously measure the atmospheric dynamics, surface energy

119

balance, radiation, chemistry, aerosols and atmospheric electricity. Here, we use only meteorolog-

120

ical observations at the CRA site which is a rural site located on a plateau in the foothills of the

121

Pyrenees. At the CRA site, standard meteorological observations have been collected since 1995.

122

More details on the P2OA observatory can be found on the website http://p2oa.aero.obs-mip.fr/.

123

(8)

Given the geographical position of the three observatories, various local processes, such as urban

124

heat islands, cloud cover, and mountain/plain breeze circulations, snow cover, and clouds have a

125

role to play concerning daily temperature anomalies.

126

b. Data used

127

In order to base our analysis on a common period with a uniform data format, data from the

128

Meteo-France standard weather station hosted by CRA-P2OA were used for this study. We em-

129

ployed hourly values concerning temperature and incoming shortwave radiation at 2 m, wind speed

130

and direction at 10 m and rainfall between 2003 and 2013. In the framework of the current study,

131

a similar quality control, homogenization and a combination of variables from various sources

132

as seen in the SIRTA-ReOBS were performed for the meteorological variables collected in the

133

C´ezeaux-COPDD and CRA-P2OA observatories.

134

To characterize the influence of large-scale circulations, we based our study mainly on daily

135

temperature anomalies at 2 m above the surface at the three observatories. To ensure that our

136

anomaly was not affected by seasonal variability in temperatures, it was defined by comparison

137

to the average of the current month. We defined the daily temperature anomalies (aT(j)) for the

138

day j by removing the 2003-2013 monthly mean temperature at each observatory. This can be

139

expressed through the following equation:

140

aT(j) =<T >j−<T >[m,2003−2013] (1)

where<T>jis the daily mean temperature for the day j, computed from the mean of hourly tem-

141

peratures. <T >[m,2003−2013]is the monthly mean temperature calculated over the entire period,

142

andmis the month represented numerically. For example,<T >[1,2003−2013]was the temperature

143

averaged over all the days in January across the period 2003-2013.

144

(9)

c. Large scale analysis diagnostics

145

1) WEATHER REGIMES

146

Weather regimes enable us to describe large-scale atmospheric circulations in a simple man-

147

ner. With this in mind, we used the classification of weather regimes used by Yiou and Nogaj

148

(2004) and based on the daily anomalies of sea level pressure (SLP) acquired from the NCEP (Na-

149

tional Center for Environmental Prediction) reanalyses (2.5×2.5) (Kalnay 1996). The weather

150

regimes are defined in the Euro-Atlantic region (80W-30E, 30-70N) (Fig. 1b, (the larger black

151

square one) and determined from the “K-means” algorithm, computed from the first 10 Empirical

152

Orthogonal Functions (EOFs) of seasonal SLP anomalies (Cheng and Wallace 1993; Michelan-

153

geli et al. 1995) from 1948 to 2014. The classification used in this study therefore depends on the

154

season. Figure 2 illustrates the four weather regimes defined in winter and their occurrence during

155

the 1948-2014 period. We note in this Figure, the positive (reg. 3) and negative (reg. 4) phases of

156

the North Atlantic Oscillation (respectively NAO+ and NAO), a “Scandinavian blocking” (reg.

157

2), and the “Atlantic Ridge” (reg. 1). Weather regimes appear with a similar frequency with a 27%

158

occurrence for NAO+and “Scandinavian blocking”. During the transitional seasons of spring and

159

autumn, a classification into weather regimes is not always appropriate due to seasonal shifts (Vrac

160

et al. 2013). Vrac et al. (2013) found that spring frequently corresponds to an early summer or a

161

longer winter, and that autumn is related to a longer summer or earlier winter, making a definition

162

of a regime during these two seasons difficult. Here, we do not consider this classification for

163

transitional seasons. It is also necessary to consider the stability of the regimes during the winter

164

and summer, as they are sometimes not well defined, and only transitory.

165

In order to eliminate the days with ambiguous classification in winter and summer, we use a

166

criterion based on the Euclidean distance and the spatial correlation from the nearest weather

167

(10)

regime deduced by the K-means method. We filter the classification by eliminating the days for

168

which the Euclidean distance from the nearest weather regime is larger than 10 hPa and with a

169

spatial correlation with the nearest weather regime lower than 0.15. We eliminated 5.2% (52 days)

170

and 10,8% (109 days) of the total days in winter and summer respectively.

171

Here, we are interested in the influence of the large-scale atmospheric regimes on the variabil-

172

ity of daily temperature anomalies (equation 1) at the three observatories. Figure 3 shows the

173

box plot of daily temperature anomalies in winter and summer for each site and for each weather

174

regime during the 2003-2013 period. This Figure indicates that in winter, NAO+yields relatively

175

milder temperatures at all sites, while NAO and blocking are characterized by relatively colder

176

temperatures at all sites. During Atlantic Ridge conditions, the occurrence of either warmer or

177

colder temperatures than those on average is relatively similar, except at SIRTA, where the winter

178

is mostly mild when this regime prevails. It is however, important to note that specific anomalies,

179

warm or cold, can occur whatever the weather regime at SIRTA, whilst very cold winter days are

180

unlikely to occur at C´ezeaux-COPDD or CRA-P2OA when NAO+ or Atlantic Ridge conditions

181

exist. Extreme temperature anomalies are more frequent at SIRTA, and variability is usually en-

182

hanced, except during NAO+. In summer, the weather regimes have almost the same effect at all

183

sites, even if the variability at C´ezeaux-COPDD is greater than at the other two sites, and extremes

184

are enhanced. At C´ezeaux-COPDD, the Atlantic Ridge and NAO+ have positive daily anomalies

185

on average in winter (0.6C and 0.2C respectively) and summer (0.6C and 1.9C respectively),

186

indicating mild and warm temperatures respectively during these two seasons. These results are

187

consistent with those of Yiou et al. (2007) in the fall/winter of 2006/2007. From these results, we

188

conclude that the weather regimes derived from the SLP data do not explain the daily temperature

189

anomalies at the three observatories in winter and summer.

190

(11)

2) LARGE-SCALE FLOW ANALOGUES

191

The slight difference in the anomaly of mean temperatures among the weather regimes in sum-

192

mer, the large variability in the daily temperature anomalies and the fact that the weather regimes

193

are not easily defined in spring and autumn, motivated us to augment the regime approach with

194

the flow-analogue method.

195

The method of atmospheric flow analogues was first introduced by Lorenz (1969). Since then, it

196

has found many applications, including weather prediction (Van den Dool 2007). Yiou et al. (2007)

197

used this approach to infer the connection between surface climate variables and atmospheric

198

circulation. In this study, we use the flow-analogue method developed by Yiou et al. (2007) and

199

used by Chiriaco et al. (2014) and Cattiaux et al. (2010) to study climate variability across Europe.

200

For each day during the eleven year period (2003-2013), we looked for days within the same

201

time series which had similar large-scale atmospheric conditions. For this, we considered field

202

anomalies of geopotential height at 500 hPa from the ERA-Interim (ERAI) reanalyses (0.75 ×

203

0.75) of European Center for Medium-Range Weather Forecasts (ECMWF) (Dee et al. 2011), a

204

typical diagnostic tool for large-scale circulations. Analogue days were found by minimizing a

205

Euclidean distance and maximizing a Spearmann correlation. More details on the flow analogues

206

method can be found in Yiou et al. (2007).

207

By using flow analogues to quantify the relative influence of the large, local, and mesoscale

208

processes on surface temperature anomalies, we considered two nested domains. The first domain

209

covers the Euro-Atlantic region (80W-30E, 30N-70N) (Fig. 1b, black square). This domain

210

is also the one used by Cattiaux et al. (2010); Vautard and Yiou (2009); Yiou et al. (2007) and

211

Chiriaco et al. (2014) to establish the link between extreme events (cold waves, heat waves and

212

drought) and large-scale conditions over Europe. The second domain covers the area 21W-30E,

213

(12)

30-60N (Fig. 1b, white square). Compared to the larger domain, this smaller domain (mesoscale)

214

weighs the influence of the Mediterranean sea on synoptic circulations more heavily than the

215

Atlantic Ocean.

216

For each day in our studied period and for each domain considered, we kept a maximum of ten

217

analogues, which satisfied the following two criteria: (i) the Spearman spatial correlation had to be

218

greater or equal to 0.6, ensuring the quality of the similarity, and (ii) they should not be closer than

219

6 days from the current day, in order to ensure that the analogues were independent of the target

220

day (assuming a decorrelation time of 3 days before and 5 days after the target day). These criteria

221

eliminated 6,4 % (around 256 days) of the days from the large domain and 3 % (around 119 days)

222

from the small domain. The scores are higher in winter, spring and autumn than in summer for

223

both domains. We found 134 and 54 unselected days respectively for the large and small domain

224

in Summer.

225

d. Analysis protocol

226

To quantify the contribution of local processes and large scale circulations at each site, we com-

227

pared the observed temperature anomalies to the temperature anomalies observed during the ana-

228

logue days. Figure 4 illustrates this approach for the year 2007 with analogues of circulation

229

computed over the small domain. It shows that, for all observatories, the analogues reproduced

230

the observed temperature anomalies quite well, but there was also a great variability between ana-

231

logues. For certain days, the analogues could not capture the amplitude of the observed anomalies,

232

as can be seen in the example from 17 to 20 January 2007 on all sites, February 2007 at SIRTA

233

and C´ezeaux-COPDD, at the end of August 2007 at CRA-P2OA, and at the end of April 2007 at

234

SIRTA. A smaller standard deviation of the ten anomalies of analogous days combined with an av-

235

erage closer to the temperature anomaly of the day in question means that the large scale explains

236

(13)

the anomaly. In our study, we investigated whether this departure from the observed series relative

237

to the envelope defined by the atmospheric conditions on analogue days can be explained by local

238

processes. Weather regimes were used to describe and better understand the large-scale influence

239

(see indications of the regimes in Fig. 4).

240

3. Analysis of large-scale conditions versus local processes

241

In order to estimate the influence of the Mediterranean Sea relative to the Atlantic Ocean at the

242

three sites, we first evaluated the ability of the analogues to represent the observed series using

243

the two different domains described above. Afterward, the difference between the observed series

244

and the temperature anomalies of the analogues was quantified by the definition and the use of

245

an anomaly index. Finally, we focused on specific periods during which the difference was larger

246

than 1.5 C, tried to identify the relevant processes, and discussed the relative contribution of

247

large-scale and local processes.

248

a. Sensitivity to the Mediterranean Sea

249

Figure 5 presents the correlation between observed anomalies and those deduced from flow

250

analogues in the large and small domains (Fig. 1b) for each site and for each season. All observed

251

daily temperature anomalies for each season are correlated with those of their 10 analogue days.

252

Thus, for each season of each year from 2003 to 2013, we have one correlation coefficient. This

253

Figure points out larger correlation coefficients in the small domain than in the large domain. This

254

is obvious for the two southern observatories whatever the season, whereas higher correlation

255

coefficients across the small domain are observed only in summer and spring for SIRTA. This

256

shows that SIRTA is more influenced by large-scale air masses coming from the Atlantic than by

257

(14)

mesoscale processes induced by orography and the presence of the Mediterranean Sea, which can

258

strongly influence the weather across southern France (e.g Ducrocq et al. (2008)).

259

We found a large spatio-temporal variability in the correlation coefficients. CRA-P2OA indi-

260

cated, on average, the lowest correlation coefficients for the two domains (0.52 and 0.35 respec-

261

tively for the small and large domain) compared to the other two sites (for the small domain,

262

C´ezeaux-COPDD and SIRTA had respectively 0.55 and 0.57 and for the large domain, 0.38 and

263

0.46 respectively). This difference can be due to the fact that CRA-P2OA is located in proximity

264

to the Pyrenees, where local processes linked with topography exist: for example, local convec-

265

tion or plain-mountain breeze circulations are more frequent in summer. The two cases of very

266

low correlation with the large domain (at the bottom-left of each subplot in Fig. 5 with green and

267

black colors) were observed in autumn 2011 at each site, during the winter of 2006 at SIRTA, and

268

during the winter of 2008 at CRA-P2OA and C´ezeaux-COPDD. The autumn of 2011 was excep-

269

tionally warm. It was indeed the second warmest autumn during the period 1948-2011, after 2006,

270

according to Cattiaux and Yiou (2012). Cattiaux and Yiou (2012) found that the flow analogues

271

underestimated the amplitude of the seasonal temperature anomaly in Europe during this specific

272

season. This suggests that global warming plays an important role by increasing the concentration

273

of greenhouse gases: the advected air mass is warmer, but it can also enhance local feedbacks.

274

In the following section, we evaluate the flow analogues approach by considering only the

275

smaller domain, in order to quantify the influence of local processes on the climate variability

276

at the three sites.

277

b. Large-scale influence

278

We have attempted to better quantify the relative contribution of large scale versus local pro-

279

cesses on the amplitude of temperature anomalies. Since the average signal of the analogues have

280

(15)

inherently lower magnitude fluctuations, we introduce Im, a new normalized index to facilitate

281

comparison of the observations and analogue series.

282

This indexIm, defined for each monthm, represents the monthly average anomaly<aT(j)>m

283

relative to the standard deviation of the 2003-2013 daily anomalies for the given monthm. We

284

computeImwith:

285

Im= <aT(j)>m q

<(aT(j)−<aT(j)>[m,2003−2013])2>m

, (2)

where<aT(j)>[m,2003−2013]is the average anomaly of temperature of the current monthmduring

286

the period 2003-2013. In other words, the red line in Fig. 4 is averaged monthly and divided by the

287

standard deviation computed from the monthly anomalies for the period 2003-2013. Concerning

288

the analogue signal, the same definition of the index is applied using all observed anomalies in the

289

analogue days.

290

Figure 6 represents the time series of this index across the period 2003-2013. The flow analogues

291

reproduce the variability of surface temperature anomalies particularly well. The correlation coef-

292

ficients betweenImfor observations and analogues are 0.80 for SIRTA, 0.85 for C´ezeaux-COPDD

293

and 0.86 for CRA-P2OA. This means that the large scale actually plays a predominant role in

294

creating the temperature anomaly variability on monthly scales, which is not surprising.

295

In Fig. 6, one may note the spatio-temporal variability ofImat the three observatories. The years

296

2003 and 2011 were the warmest years at every site for the period 2003-2013, whereas the coldest

297

year at every site was that of 2010 with negativeImfor every month.

298

While the general trend is well captured by Im for analogue days, the magnitude of certain

299

events is not reproduced. For example, February 2007 was exceptionally warm with Im larger

300

than 1.7 at SIRTA and C´ezeaux-COPDD according to observations. This peak in temperature

301

is not reproduced by flow analogues with an index of around 0.5 (Fig. 6) when using the small

302

(16)

domain, and is even negative when using the large domain (not shown). The large anomaly is not

303

observed at CRA-P2OA. The spatial variability of temperature anomalies during this winter and

304

the difference between observed anomalies and analogues allow us to hypothesize that specific

305

synoptic-scale features leading to local anomalies that are not resolved by the analogue approach

306

alone and that local processes may have played a specific role at each site during this period.

307

c. Analysis of specific events during winter 2007

308

We focused on the winter of 2006/2007 in order to further investigate the contribution of large

309

and local-scale processes on the spatio-temporal variability of daily temperature anomalies at the

310

observatories. Note that winter 2007 appears to be the warmest of our study period: it was the sec-

311

ond warmest winter in France since 1959 according to climatology established by Meteo-France

312

(http://www.meteofrance.fr/).

313

Figure 7 shows the time series of daily temperature anomalies for the winter of 2006/2007

314

from observations and analogues. It focuses in on the period from January to February 2007 in

315

Fig. 4. During this period, two regimes, “NAO+” and ”Atlantic ridge” are persistent. “NAO+” is

316

associated with a southwesterly flow over Northern Europe (Michelangeli et al. 1995). We showed

317

in section 2c that the two regimes, “NAO+” and “Atlantic Ridge” are usually the warmest in winter

318

at all three sites. These results are consistent with those of Yiou et al. (2007) for the exceptionally

319

warm 2006/2007 fall/winter. The regime NAOappears between 22 and 26 January, with negative

320

anomalies at all sites. Snow was observed at SIRTA on 23 January, and from 23 to 25 January at

321

CRA-P2OA and C´ezeaux-COPDD.

322

We focused on specific warm events during the winter of 2007 to investigate the role of lo-

323

cal processes on the spatio-temporal variability of daily temperature anomalies. We will further

324

analyze two periods /dates: the period 17 to 19 January and a single day: 16 February 2007.

325

(17)

1) 17-19 JANUARY 2007CASE

326

The period from 17 to 19 January encompasses the warmest anomalies of the month of January

327

2007 at all sites (Fig. 7) with spatial variability in the amplitude: the southern site (CRA-P2OA)

328

shows the lowest daily temperature anomalies compared to the other two sites (warmest anomaly

329

of 9.4, 10 and 7.2 C at SIRTA, C´ezeaux-COPDD and CRA-P2OA respectively, on 18 January

330

2007). The observed positive temperature anomalies are higher than those of analogue days for

331

the whole 17-19 January period at SIRTA and C´ezeaux-COPDD and only at CRA-P2OA for the 18

332

January. Despite the spatial variability in the temperature anomalies, 18 January 2007 indicates an

333

anomaly on a large scale and one can wonder why the anomaly’s amplitude of such a large-scale

334

event is not reproduced by any of the analogue days.

335

To answer this question, the large-scale meteorological situation of analogue days is verified

336

using satellites and ERAI reanalyses and local effects are analyzed based on the meteorological

337

history of the surface measurements and radiosoundings. The meteorological history provides a

338

view of the atmospheric conditions of previous days on a local scale. We consider, therefore,

339

the diurnal cycles on 18 January 2007 and on the two previous days (16 and 17 January 2007)

340

to point out the effect of the ‘‘local meteorological history’’ at each site. Similarly, the ‘‘local

341

meteorological history’’ of the five best analogue days on 18 January 2007 is presented. For

342

example, if 20 December 2011 is one analogue day for 18 January 2007, the time series from 18

343

to 20 December 2011 are displayed.

344

The large-scale circulation is the NAO+ regime on 17 and 18 January, and ‘‘Atlantic ridge’’

345

on 19 January (Fig. 7). Figure 8 shows the wind speed and direction at 600 hPa from the ERAI

346

reanalyses. It indicates an increasing westerly wind over France during the 16-18 January period.

347

The five most accurate analogues are generally similar with an increasing wind speed from 17

348

(18)

to 18 January and show similar wind directions. On 16-17 January, only one analogue indicates

349

similar wind speed and direction. However, wind speed varies from one analogue to another.

350

The reflectance in the visible channel at 0.6µm of the MeteoSat Second Generation (MSG) at

351

1300 UTC on 18 January 2007 is shown in Fig. 9a. Significant cloud cover over the North Atlantic

352

and Europe was observed with a window of clear sky over the Mediterranean basin, the South of

353

Spain and the Pyrenees region. Similar cloud cover was also observed on 17 and 19 January

354

2007 (not shown). The method of Wang and Rossow (1995) was applied to the vertical profile of

355

relative humidity from the radiosoundings at Trappes on 18 January (Fig. 9b) to define the cloud

356

base height. Wang and Rossow (1995) used among other criteria, 87% and 84% as maximum and

357

minimum relative humidity thresholds respectively and relative humidity jumps exceeding 3% at

358

cloud-layer top and base to characterize a cloud-layer. With this method, we find in Fig. 9b that

359

on the 18 January, cloud cover was dominated by low-level clouds with a base not exceeding 700

360

m in height at 1100 UTC. At 2300 UTC, cloud cover descended and thickened. Based on the

361

Meteo-France weather service station, drizzle was observed that night, with 0.8 mm falling at this

362

site. Combining the satellite image and vertical profiles of relative humidity, we find that these low

363

clouds were stratocumulus clouds associated with the stable atmospheric conditions in Southern

364

Europe linked to the NAO+ regime. Indeed, the stratocumulus clouds occur widely over Europe

365

in January, according to Hahn and Warren (2007). A similar analysis of the vertical profiles of

366

relative humidity for the five most accurate analogue days (Fig. 9b) shows that 18 January 2007

367

was the cloudiest day: either there was no cloud cover (analogue day number 3), or there was cloud

368

cover which disappeared between 1100 and 2300 UTC (analogue day number 1), or much thinner

369

cloud cover (analogue days number 4 and 5). We can expect an effect due to this cloud layer on

370

18 January since it impacts the radiative budget at the surface at SIRTA and C´ezeaux-COPDD.

371

(19)

The meteorological history of 18 January and its five most precise analogue days was analyzed

372

with surface measurements. The large scale cloud cover, discussed previously (Fig. 9), impacts

373

incoming solar radiation (ISR) (Fig. 10). The ISR measured at the surface increases from north

374

to south, with very cloudy conditions at SIRTA for every day and almost no reduction of ISR

375

at CRA-P2OA. The integration of ISR across the three days defining the meteorological history

376

period (not shown) demonstrates low levels of ISR for the observed days compared to the analogue

377

days at SIRTA and C´ezeaux-COPDD, contrary to CRA-P2OA.

378

Figure 10 presents the time series of temperature, incoming shortwave radiation at 2 m, wind

379

speed and direction at 10 m above the ground. Cloud cover also clearly impacts the diurnal cycle

380

of 2m-temperature (Fig. 10); Low-level cloud cover at SIRTA reduces the cooling of the earth and

381

damps the diurnal temperature cycle. This is also the case at C´ezeaux-COPDD, on 18 January.

382

On the contrary, a large diurnal temperature cycle can be observed at CRA-P2OA on most of the

383

days, especially during the period 16-18 January.

384

At SIRTA, the westerly wind direction at the surface is consistent with the synoptic wind (Fig. 8).

385

The wind direction at C´ezeaux-COPDD is quite variable but maintains a westerly direction on av-

386

erage, whereas a clear effect of the mountain range can be observed on 16, 17 and some of 18

387

January at CRA-P2OA, with some north-easterly slope winds during the day and southerly at

388

night, a sign of the plain-mountain diurnal circulation. Figure 10 shows the diversity of the con-

389

ditions observed during the analogue days at CRA-P2OA, which makes the comparison difficult.

390

Among the five most accurate analogue days, only three are cloud-free. All of them indicate a

391

reversal of the wind direction twice a day. This is characteristic of the slope wind, which seems

392

to play an important role and blurs the comparison of the diurnal cycle. During winter, a lack of

393

cloud cover may allow weak convection over mountains, and certainly greater radiative cooling

394

at night. This southerly mountain breeze during the night advects cool air from the mountains

395

(20)

and is associated with low temperatures at night. The mountain breeze which occurs during the

396

NAO+ regime could then reduce the positive temperature anomaly tendency associated with this

397

regime. The meteorological history of 18 January shows a slope wind regime until noon, when a

398

clear westerly wind settles at the surface. From that moment, the temperature clearly increases,

399

and remains high during the night, with no mountain breezes, between 18 and 19 January. The

400

daily mean temperature then leads to a larger positive temperature anomaly compared with the

401

analogue days with slope winds lasting all day.

402

From these large and local-scale analyses of the observed days and their analogue days, we

403

can ascribe this positive temperature anomaly to a large-scale event observed at the three sites.

404

The NAO+ regime, which advects mild temperatures from the Atlantic ocean, is characterized

405

by the warmest temperature anomaly in winter (Fig. 3). The flow analogue method shows some

406

limitations, however, in representing this event. The cloud layer is particularly low and deep,

407

and lasts for three days over the northern part of France, whereas nothing in the meteorological

408

history of the analogue days indicates such conditions. This cloud cover could imply a warming

409

radiative effect over SIRTA and C´ezeaux-COPDD during the 17-19 January period, which would

410

amplify the positive anomaly due to what is already mild air advection. While the low cloud

411

cover observed during this event is not a local effect, its radiative interaction with the surface is

412

dependent on surface temperature and can be considered a local effect.

413

In conclusion, it seems that this abnormal warm event stands out from the analogue days, for

414

various reasons at SIRTA and C´ezeaux-COPDD in the first instance and then at CRA-P2OA.

415

The large-scale positive anomaly associated with the NAO+ regime is amplified at SIRTA and

416

C´ezeaux-COPDD by the warming radiative effect of an unusually low cloud cover occurring over

417

the two sites during the 11 year period. This event, lasting for three days, lead to warmer anomalies

418

than on analogue days. Meanwhile, in CRA-P2OA, the absence of clouds lead to a down-valley

419

(21)

wind regime which tends to cool the air at night and to reduce the NAO+ regime warm anomaly.

420

The down-valley wind was observed on 18 January until midday and did not occur the following

421

night. This led to higher nocturnal temperatures and warmer daily temperature anomalies than on

422

analogue days the following night. These results show that radiation and cloud cover are important

423

predictors of daily temperature anomalies in winter at this observatory.

424

2) 16 FEBRUARY2007CASE

425

16 February 2007 is an example of a case where the temperature anomaly largely exceeded the

426

range of the flow analogues at a single site. A strong and warm anomaly of 12.3C was observed

427

at CRA-P2OA on that day, while all analogues showed an anomaly below 8C (Fig. 7). At the two

428

other observatories, the temperature anomaly on this day was within the envelope of the analogues.

429

The synoptic atmospheric conditions on 16 February were forced by the presence of very low

430

pressure centered over Iceland, and its associated thalweg extending from the island towards the

431

south, near Spain and Morocco. This situation, which often announces the arrival of a front,

432

generated a south-southwesterly wind regime in altitude, bringing dry and warm air from the

433

south. The wind at 600 hPa across the three sites and deduced from the reanalyses of the European

434

Center is shown in Fig. 11 for 16 February and for its analogous days. The analogues have the

435

same types of southwesterly wind regime across the three sites. This situation generally leads to a

436

positive temperature anomaly due to the southern origin of the air mass in many such cases. For

437

this reason, on average, the envelope of the analogues shows a positive temperature anomaly at all

438

sites (Fig. 7).

439

Southerly winds over the ridge of the Pyrenees correspond to the typical situation of the so-

440

called foehn phenomenon: the east-west orientated mountain ridge is an obstacle for the flow,

441

which can be partially blocked in the lower layers and which can bypass the ridge, with the flow

442

(22)

splitting at its sides, or/and passing over and through it across the mountain passes (Scorer 1949,

443

1953, 1955; Scorer and Klieforth 1959; Seibert 1990; ´Olafsson and Bougeault 1997; Jiang et al.

444

2005). The adiabatic descent of air in the lee, usually occurring together with the flow over the

445

mountain, is associated with a typical drying and warming in the lower lee air layers on the French

446

side (‘foehn effect’).

447

One of the most important governing variables for this phenomenon is the upwind wind profile,

448

and particularly the upwind component, which is perpendicular to the ridge: the larger this com-

449

ponent, the easier it is for the flow to go over the mountain and generate the foehn effect (Seibert

450

1990). For the Pyrenees in the vicinity of the CRA-P2OA site, we evaluate the cross-component

451

at 210 azimuth (±10): that is, a wind with this direction (which is very similar to a southerly

452

wind) travels exactly transversely to the ridge, on a 150 km horizontal scale. This direction is

453

also aligned with the main Aure Valley, which is situated south of the CRA-P2OA observatory

454

and North-South orientated. Figure 12a shows the upwind profiles of the cross-ridge component

455

(projection of the wind on the 210 axis), for 16 February and for all analogues, at 0000 UTC.

456

These are deduced from the radiosoundings launched daily from Zaragosa in Spain. Zaragosa is

457

located about 150 km south of the ridge of the Pyrenees, and 200 km from the CRA-P2OA site.

458

These profiles confirm the potential to generate the foehn effect at CRA-P2OA for most of the days

459

shown, as this component is positive for most cases above 1000 m. It also reveals that 16 February

460

is the case with the strongest 210 upwind component between 1000 m and 6000 m, especially

461

below 3500 m, making it the most favorable case for a strong foehn event (the highest peak in the

462

Pyrenees is at 3400 m). Figure 11 also shows a significant increased in wind speed upwind of the

463

ridge during the day.

464

Figure 12b is a the visible image of MSG at 1500 UTC on 16 February 2007. This day was

465

marked by large cloud cover over the western Atlantic and northern Europe, and a clear sky above

466

(23)

the Mediterranean basin and eastern Europe. Cloud cover over the Pyrenees shows that the sky

467

was clear in Spain and in the lee of the mountain (where CRA-P2OA is situated). Farther to the

468

north, a cloud with a well-defined southern border, typical of the upward branch of a mountain

469

wave, can be observed, and is usually associated with foehn and southerly overpassing flows. The

470

clear sky in Spain reveals a ‘‘dry foehn’’ as opposed to some cases, where clouds are blocked on

471

the Spanish side, with some rain that can contribute to the drying and warming effect of the air in

472

the lee on the French side. This means that on 16 February, air mass was generally very dry at the

473

large scale, a fact which is confirmed by the radiosoundings taken at Zaragosa, Bordeaux (Atlantic

474

French coast), Trappes (close to Paris), and the synoptic situation discussed before. The Trappes

475

soundings at 1100 and 2300 UTC show very dry and warm air between 800 m and 4000 m. Above

476

this altitude, fine medium clouds (of about 500 m) are observed (not shown).

477

We can now consider the observations at the surface of the different observatories. Figure 13

478

presents the evolution of the meteorological variables observed close to the surface on 16 February

479

2007, and its analogues. The most striking feature is found in the surface wind at CRA-P2OA: for

480

all the analogues, the wind at the surface is southerly during the night and northerly during the day.

481

This, along with the low associated wind speed (below 6 m s−1), is indicative of the mountain-plain

482

diurnal circulation. That is to say, although the upwind flow is from the south, and sometimes has

483

a strong wind speed (Fig. 12a), this does not prevent the plain-mountain circulation from setting

484

up during those analogue days. It is actually quite classic, with the southerly wind kept at a higher

485

level. Note that this does not prevent the foehn effect (warming and drying in the lee), or the

486

warmer local temperature that can be found at this site relative to the other sites. On 16 February,

487

however, the wind at the surface of CRA-P2OA remained southerly all day, with the wind speed

488

increasing during the day, by up to 10 m s−1 at times. This means that for this specific day, the

489

upwind flow was strong enough to be able to create a downslope wind throughout the entire day in

490

(24)

which case, the warming and drying effect in the lee is still larger. This is consistent with Fig. 12a,

491

which shows the characteristics of this day in terms of upwind conditions. It probably explains

492

most of the temperature anomalies found at CRA-P2OA, which exceed the usual anomalies found

493

in analogous synoptic situations (Fig. 7).

494

At C´ezeaux-COPDD, this synoptic situation does not lead to a marked anomaly, but the general

495

dry and warm air leads to a large diurnal increase. The night of 16 to 17 February may have been

496

influenced by a small foehn effect, in the presence of westerly winds (typically occurring in the

497

‘‘Chaine des puys’’ mountains to the west of the site). The air temperature does not decrease

498

much, and the wind continues to arrive from the west. At SIRTA, the wind at the surface is

499

easterly, surprisingly, while the sounding at Trappes shows a strong southerly flow down to the

500

lowest levels of the atmosphere. This weak easterly wind at SIRTA seems unconnected to the

501

warm, dry southerly air above, and could explain the relative lower temperature found on 16

502

February (relative to its analogues).

503

This event shows how meso-β scale processes linked with orography can amplify a temperature

504

anomaly which is primarily forced at the synoptic scale. This specific type of amplification has

505

been previously observed by Takane and Kusaka (2011) in Japan in the summer.

506

4. Summary and Conclusions

507

This study aimed to evaluate the relative contribution of large-scale atmospheric circulation and

508

more local processes to daily temperature anomalies over a north-south transect of France. The

509

study was based on the observations of meteorological variables at three observatories and on

510

NCEP and ECMWF reanalyses. The flow analogues method was used in particular to diagnose

511

the fingerprint of the large-scale synoptic circulations concerning the temperature anomaly, and to

512

highlight the potential role of local processes in inhibiting or amplifying the anomaly.

513

(25)

The analysis of weather regimes over the Euro-Atlantic region shows that the large-scale atmo-

514

spheric circulations have an important influence on the daily temperature anomalies at the three

515

observatories in winter. The “NAO+” and “Atlantic Ridge” appear to be the warmest regimes in

516

this season. While the influence of the four weather regimes on daily temperature anomalies does

517

not statistically differ at the three observatories in the summer due to strong variability within each

518

regime, extreme anomalies are associated with one or two regimes at all observatories except for

519

that of SIRTA.

520

The flow analogue approach applied over two different domains shows that SIRTA is less af-

521

fected by the mesoscale processes formed around the Mediterranean Sea than the other two obser-

522

vatories, which is not surprising considering its northern location.

523

The atmospheric circulation analogue method demonstrates the large correlation between a

524

monthly temperature anomaly index calculated from the observed series and that which is pro-

525

vided by the representation of the analogues. This highlights the predominant role played by the

526

large-scale situation in the temperature anomalies. Sometimes, however, the amplitude of the

527

monthly temperature index is not captured by the flow analogues and shows a large spatial vari-

528

ability between the three observatories. It is suggested that these discrepancies are related to local

529

processes. Two specific events revealed in the warmest winter in the period 2003-2013 are further

530

analyzed to test this hypothesis: 1) the 17-19 January 2007 event which had the strongest posi-

531

tive temperature anomaly at the two northern observatories (SIRTA and C´ezeaux-COPDD) and,

532

2) the 16 February 2007, for which only CRA-P2OA indicated a very large positive temperature

533

anomaly, found beyond the signal of the set of analogues.

534

From the analysis of these two events, the impact of several local processes have been identified:

535

(26)

1) the local impact of non-local cloud cover during westerly wind conditions in winter: low-level

536

clouds have been shown to increase the positive temperature anomaly at SIRTA and C´ezeaux-

537

COPDD in these conditions, partly due to the positive radiative green-house effect of the clouds.

538

2) the orographic impact: CRA-P2OA and C´ezeaux-COPDD are both in proximity to mountains

539

and are frequently impacted by either foehns or slope wind effects. In a weak large-scale situation,

540

the slope breeze easily settles at CRA-P2OA, and can transport cool air from the mountains during

541

the night in winter. Foehn events observed at both the CRA-P2OA and C´ezeaux-COPDD sites with

542

southerly and westerly wind conditions respectively, can amplify positive temperature anomalies,

543

originally forced by large scales.

544

The analysis of two specific events reveals that some local processes are able to modulate the

545

trend of the daily temperature anomaly driven by the large-scale atmospheric circulation. How-

546

ever, such a phenomenological approach remains difficult, since the understanding of one event

547

necessitates the analysis of the meteorological history of not only the event itself, but also of its

548

analogue days. To investigate the impact of local processes, a systematic study of all cases in

549

which observations differ from analogue days would be necessary.

550

Departures between observed local anomalies and analogues might not only be due to local

551

processes but also to differences between the observed event and its analogues on the synoptic

552

scale, which would not be adequately resolved by the classical analogue approach employed. A

553

possibility for the investigation of this is the combining of different variables in the analogues

554

method (vorticity, water vapor, temperature, wind). Even if this would require much longer series

555

in order to ensure a large enough number of analogues for each day.

556

Acknowledgments. This work was carried out in the context of ROSEA, and funded by AL-

557

LENVI. The ROSEA program now belongs to a larger program and national network called AT-

558

(27)

MOS (Atmospheric Short-Lived Climate Forcers Observing System). The administrative and

559

technical supervision of the observatories have been acknowledged. Part of the data used here

560

were collected at the Pyrenean Platform for Observation of the Atmosphere P2OA, Observa-

561

toire de Physique du Globe de Clermont Ferrand OPGC and Site Instrumental de Recherche par

562

T´el´ed´etection Atmosph´erique SIRTA. P2OA facilities and staff were funded and supported by the

563

Observatoire Midi-Pyr´en´ees (University of Toulouse, France) and the CNRS (Centre National de

564

la Recherche Scientifique) INSU (Institut National des Sciences de l’Univers). OPGC facilities

565

and staff were funded and supported by the Blaise Pascal University of Clermont Ferrand and

566

CNRS (Centre National de la Recherche Scientifique) INSU. We are grateful to NCEP, ECMWF,

567

and Meteo-France for providing the observation data and global model reanalyses used in this

568

study. We acknowledge the CNES for partially funding M. Chiriaco’s research. P. Yiou was sup-

569

ported by an ERC advanced grant (No. 338965 - A2C2 ). The authors would like to thank the three

570

anonymous reviewers for their fruitful comments, which helped us to improve the manuscript. Fi-

571

nally, we thank Naomi RIVIERE and Eric PARDYJAK for carefully proof reading our manuscript.

572

References

573

Bastin, S., M. Chiriaco, and P. Drobinski, 2016: Control of radiation and evaporation on tem-

574

perature variability in a wrf regional climate simulation: comparison with colocated long term

575

ground based observations near paris.Climate Dyn., doi:10.1007/s00382-016-2974-1.

576

Bo´e, J., and L. J. Terray, 2014: Land-sea contrast, soil-atmosphere interactions and cloud-

577

temperature interactions: interplays and roles in future summer european climate change.Cli-

578

mate Dyn.,42(3-4), 683–699.

579

Références

Documents relatifs

stacking fault energy by doping GaAs was found up to 1273 K ; no clear influence of the temperature. was found in spite of what is expected

Abstract : Plastic deformation tests have been performed at low temperature (T&lt;450 C) under a confining pressure in order to promote dislocation motion at temperature where

1) At the melting point the resonance signal drops to an unmeasurable small value in a very limited temperature interval. Line broadening by diffusion could not be

La reine était terrifiée; Et le prince qu'il aimait Cent joie se réjouiront dans l'âme,. Il est tombé en dessous de son

A series of electrooptic effects associated with the change of crystal orientation and local director in the lattice [5-9], electrostriction [9-1Ii and phase transitions [10-15]

cooperative growth, leads to highly non-trivial behavior: arbitrary Turing machine simulation [11, 19], efficient production of n × n squares and other simple shapes using Θ(log n/

axisyrnmetric notched tensile specimen. 2) A simple 2-D quasistatic FEM model of the instrumented Charpy impact test is sufficient for application of the Beremin model at

Equation (1) also allows to calculate the values of hardness at various temperatures by introducing the linear approximation of temperature dependence of ∆G at (T), i.e. 3a shows